Method and apparatus for squelch gating a receiving signal
13 claims: 9 independent, 4 dependent
- 1Claims 1. Method for squelch gating a receiving signal depending on the level of phase noise in said receiving signal comprising following steps:• determining sampled amplitudes (7n״) and sampled phases (φ η ) of said receiving signal ( x n ) , • determining sampled phase noise (p n ) by differentiating subsequent sampled phases (φ״)> • determining a squelch signal (s n ) by rectifying and averaging said sampled phase noise (p n )r • determining a start point ( SP G} , SP G2 , SP G3 , SP G4 ) of gating after a rising of said squelch signal (s n ) above a. higher threshold (S high ) delayed by a first delay time (T D] ) and determining a end point ( EP G] , EP G2 , EP G3 , EP G4 ) of gating after a dropping of said squelch signal (s n ) below a lower threshold (S ll/W ) delayed by a second delay time (T D2 ) and • gating said sampled amplitudes (7w״) from said start point ( SP Gl , SP G2 , SP G3 , SP G4 ) of gating until said end point ( EP gx , EP g2 , EP g3 , EP G4 ) of gating.
- 6Method for gating a receiving signal according to claims 1. to 5, wherein that said gating is continuously increased from an inactive gating level up to an active gating level during G:\CP12K\Letler Module\LeuersByUsers\P\2006\P30489\20061227_1657־_LTU Unterlagen, uspnjngiich_P30489_EP.c a first fading time (T fadeX ) beginning at said start point of gating (SP G3 ) respective ending at said start point (SP G4 ) of gating and is continuously decreased from said active gating level down to said inactive fading level during a second fading time (T fade2 ) beginning at said end point of gating (EP G3 ) respective ending at said end point (EP G 4) of gating.
- 7Method for gating a receiving signal according to claims 1 to 6, wherein that in case of said rising squelch signal (s n ) being below said higher threshold (S hilih ) the value of said squelch signal (s n ) is changed to the value of said higher threshold (S high ) and in case of said dropping squelch signal (s n ) being above said lower threshold (S low ) the value of said squelch signal (s n ) is changed to the value of said lower threshold (S low ).
- 8Apparatus for squelch gating a receiving signal depending on the value of phase noise in said receiving signal comprising a unit (1) for determining sampled amplitudes (/ ״ מ) and sampled phases (φ η ) of said receiving signal ( x n ) , a unit (3) for determining sampled phase noise (/?״) by differentiating subsequent sampled phases {φ״), a unit (7,8) for determining a squelch signal (s n ) by rectifying and averaging said sampled phase noise (p״), and a switching unit (10) for gating said sampled amplitudes (m״) from a rising of said squelch signal (s n ) above a higher threshold (S high ) delayed by a first delay time (T DX ) until a dropping of said squelch signal (s n ) below a lower threshold ( S law ) delayed by a second delay time ( T D2 ) .
- 9Apparatus for gating a receiving signal according claim 8 further comprising a delay unit (12) for delaying said sampled amplitudes (m n ), which is preceded said switching unit (10) . G:\CPl2K\Letter Module\LettersByUsers\P\2006\P30489\2006I227_16-57_UU Unterlagen, uspriinglich_P30489_EP.c
Independent claims9
103 paragraphs in 1 section, as filed
Method and apparatus for squelch gating a receiving signal
The invention relates to an apparatus and a method for squelch gating a receiving signal.
In digital receivers the possibility to mute an audio output signal in case of disappearance of the carrier of the received audio signal or in case of a drop of the signal-noise-ratio in the received audio signal below a threshold is known from US 6,047,170 A.
The technical realisation for determining the measure of noise in a received signal is called squelch and is based on the continuous measuring of phase noise in the audio signal and the gating of the demodulated audio signal according the measured level of phase noise in comparison with specified thresholds.
Fig. 1 shows an apparatus for gating a received audio signal on the basis of a squelch signal characterising the measure of phase noise in the audio signal.
The received sampled RF audio signal x<sub>n</sub> with its sampled cartesian components - sampled real component Re{x״} and sampled imaginary component Im{x״} - is converted in a Cordic-unit 1 to its polar components, sampled amplitude m<sub>n</sub> and sampled phase φ<sub>η</sub> . In a differentiating unit 3 of a squelch detector 3 a sampled phase difference Δφ<sub>η</sub> between a sampled phase φ<sub>η</sub> and its succeeding sampled phase φ<sub>η</sub>_<sub>λ</sub> determined in a delay unit 4 of the differentiating unit 3 on the basis of the sampled phase φ<sub>η</sub> - is determined in subtracting unit 5 of the differentiating unit 3.
The sampled phase difference Δφ<sub>π</sub> contains signal portions of low frequency, caused by frequency offset or frequency drift of the carrier in the received RF audio signal, and phase noise as signal portions of high frequency. To eliG:\CPl2K\Letter Module\LettenByUsers\P\2006\P30489\2006l227J6-57_UU Unterlagen, usprtnglich_P30489_EP c minate the signal portions of low frequency in the sampled phase difference Δφ<sub>η</sub> a subsequent highpass filter 6 of the squelch detector 2 - typically a 4<sup>th</sup> order HR highpass filter - produces sampled phase differences Δφ<sub>η</sub> comprising only phase noise relevant signal portions.
The signed sampled phase differences Δφ<sub>η</sub> corresponding to phase noise are rectified in a subsequent squaring unit 7. The squaring unit 7 can alternatively be replaced by a device performing the absolute value of its input signal. For averaging the sampled unsigned RF phase differences p<sub>n </sub>over time a digital filter 8 having a proportionalintegral characteristic concerning equation (1) represents the last signal processing unit of the squelch detector 2 delivering the sampled squelch signal s<sub>n</sub> at its output. In equation (1) f<sub>s</sub> represents the sampling rate and τ represents the time constant of the integral characteristic of the digital filter 8.
T
The sampled amplitudes m<sub>n</sub> of the RF receiving audio signal x are demodulated in a demodulator 9. The demodulated
ח audio signal y<sub>n</sub> is gated in a subsequent gating unit 10 on the basis of the determined sampled squelch signal s<sub>n</sub> and a specified threshold delivering a muted audio signal a<sub>n </sub>to the outputting unit 11.
In an off->on-»off-cycle of an audio transmission Fig. 2 displays the DC component of the carrier DC(m<sub>n</sub>) (curve 40), the rectified RF phase noise p<sub>n</sub> (curve 20) and the squelch signal s<sub>n</sub> (curve 30) in the apparatus for gating a received audio signal according to Fig. 1, whereby the time constant τ of the integrating digital filter 8 ms is 5 ms.
The time constant of the digital filter is typically between 5 ms and 10 ms. Thus random peaks in the RF phase noise p״ being shorter than 5 ms to 10 ms are not averaged
G:\CPI2K\Letter Module\LettersBy(Jsers\P'2006\P30489\2006l227J6-57_UU Unlerlagen, usprunglich_P30489_EP.c by means of the digital filter 8 with proportional-digital characteristic leading to a squelch signal s<sub>n</sub> with random peaks. Such peaks in the squelch signal s<sub>n</sub> drops below respectively rises above the specified threshold(s) and 5 disadvantageously mutes the received audio signal for a short period. Especially in case of a squelch signal s<sub>n </sub>rising above respectively dropping below a specified threshold leading to switch off respectively switch on of the received audio signal random peaks in the squelch 10 signal s<sub>n</sub> occurring shortly after the switch reverses the switch of the received audio signal.
Prolongation of the time constant τ of the integrating digital filter 8 for avoiding such unwanted reversals of . 15 switches in the audio signal in case of peaks in the squelch signal would deteriorate the time behaviour of the integrating digital filter and thus the time behaviour of the squelch detector. The worse reaction of the integrating digital filter would unwontedly delay the 20 squelch signal s<sub>n</sub> in comparison with an on-»off-step or an off-»on-step of the carrier in the audio transmission (see in Fig. 2 the delay of the squelch signal s<sub>n</sub> (curve 20) in comparison with an off—>on -step of the DC component of the carpier DC(m<sub>n</sub>) (curve 40) ) .
The object of the invention is to develop an apparatus and a method for squelch gating a received audio signal and whereby avoiding the occurrence of short-time reversal of the audio signal's switching without deteriorating the 30 time behaviour of the squelch detector.
The object is solved by a method with the features of claim 1 and an apparatus with the features of claim 8. The dependent claims comprise further developments of the 35 invention.
Inventively the start point resp. the end point of gating the audio signal is the time point, when the squelch signal s<sub>n</sub> rises above the higher threshold delayed by a first
G:\CPI2K\Letter Module\LellasBy(Jsers\P\2006\P30489\2006l227_l6-57_UU Unierla8en, usprtjnglich_P3O489_EP.c delay time resp. drops below the lower threshold delayed by a second delay time. Therefore short-time reversal of ft switching the audio signal in case of occurrence of peaks in the squelch signal shortly after switching the audio signal can be advantageously prohibited.
In a first embodiment of the inventive method a third delay time for delaying the sampled amplitudes m<sub>n</sub> of the audio signal at the start point of gating and a fourth 10 delay time for delaying the sampled amplitudes m<sub>n</sub> of the audio signal at the end point of gating is calculated to compensate the unwanted delay in the muting of the demo$ dulated audio signal y<sub>n</sub> caused by the first delay time at the start point of gating resp. by the second delay time at the end point of gating.
A delaying of the sampled amplitudes m<sub>n</sub> of the audio signal by different delay times - third delay time at the beginning of gating, fourth delay time at the end of gating - can not be realised. Thus the maximum delay time of the third and fourth delay time is chosen for delaying the sampled amplitudes m<sub>n</sub> of the audio signal both at the start and at the end of gating. The selection of one of the third or fourth delay time for delaying the sampled ך amplitudes m<sub>n</sub> of the audio signal leads to a failure in the correct time point either for starting or for ending the gating. To eliminate this failure at one of the two time points both the first and the second delay time are recalculated by the chosen maximum delay time for delaying 30 the sampled amplitudes m<sub>n</sub> of the audio signal.
For avoiding the delay between the squelch signal s<sub>n</sub> and the demodulated audio signal y<sub>n</sub> caused by the time constant r of the integrating digital filter 8 the user of 35 the receiver or an automatic selection unit can select a first time interval Δ/ relative to the original start point of gating - the time point, when the squelch signal s<sub>n</sub> rises above the higher threshold delayed by the first delay time - for determining a new start point of gating
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and a second time interval Δζ״ relative to the original end point of gating - the time point, when the squelch signal s<sub>n</sub> drops below the lower threshold delayed by the second delay time - for determining a new end point of 5 gating. The new start point of gating and the new end point of gating is determined empirically by the user or the automatic selection unit changing the first time interval Δί resp. the second time interval &t<sub>ep</sub>, until phase noise disappears at the beginning resp. at the end 10 of the audio receiving.
In a second embodiment of the inventive method a third delay time for delaying the sampled amplitudes m<sub>n</sub> of the audio signal at the start point of gating is calculated as 15 the difference of the original start point of gating and the new start point of gating being the summation of the first delay time and the first time interval Δί<sub>χρ</sub> relative to the original start point of gating. Consequently a fourth delay time for delaying the sampled amplitudes m<sub>n </sub>20 of the audio signal at the end point of gating is calculated as the difference of the original end point of gating and the new end point of gating being the summation of the second delay time and the second time interval Δζ<sub>ρ </sub>relative to the original end point of gating.
To eliminate the failure caused by delaying the sampled amplitudes m<sub>n</sub> of the audio signal both at the beginning and also at the end of gating both the first and the second delay time are recalculated each by subtracting the 30 first time interval Δί<sub>χρ</sub> resp. the second time interval Δί<sub>ΰρ </sub>from the chosen maximum delay time for delaying the sampled amplitudes m<sub>n</sub> of the audio signal.
For avoiding unwanted clicks at the beginning and/or at 35 the end of audio transmission the gating is continuously increased from an inactive gating level up to an active gating level during a first fading time T<sub>/(M</sub> at the beginning of gating and is continuously decreased from an active gating level down to an inactive gating level
G:\CPl2K\Letter Module\LettersByUsers\P\2006\P30489\20061227_1657־_UU Unterlagen, usprijnglich_P3O489_EP.c during a second fading time Tj-<sub>ade2</sub> at the end of gating. In a third embodiment of the inventive method the start point of gating is the start point of fading from the inactive level and the end point of gating is the start point of fading from the active gating level. In a fourth embodiment of the inventive method the start point of gating is the end point of fading at the active gating level and the end point of gating is the end point of fading at the inactive gating level.
Optionally for reducing the delay between the squelch signal s<sub>n</sub> and an on->off-step or an off->on-step of the carrier signal in the audio transmission the value of said squelch signal s<sub>n</sub> is changed to the value of the higher threshold in case of a rising squelch signal s<sub>n</sub> being below the higher threshold and the value of said squelch signal s<sub>n</sub> is changed to the value of the lower threshold in case of a dropping squelch signal s<sub>n</sub> being above the lower threshold.
An embodiment of the inventive apparatus and the four embodiments of the inventive method for gating a receiving signal will be described in detail in relation to the drawing. The figures of the drawing show:
Fig. 1 a block diagram of an apparatus for gating a receiving signal,
Fig. 2 a time diagram of RF phase noise, of squelch signal and of DC component of the carrier in an apparatus for gating a receiving signal according to Fig. 1,
Fig. 3 a block diagram of an inventive apparatus for gating a receiving signal,
Fig. 4 a flowchart of an inventive method for gating a receiving signal,
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Fig. 5 a time diagram of starting a gating of a receiving signal in a first embodiment of the invention,
Fig. 6 a time diagram of starting a gating of a receiving signal in a second embodiment of the invention,
Fig. 7 a time diagram of starting a gating of a receiving signal in a third embodiment of the invention,
Fig. 8 a time diagram of starting a gating of a receiving signal in a fourth embodiment of the invention,
Fig. 9 a time diagram of ending a gating of a receiving signal in a first embodiment of the invention,
Fig. 10 a time diagram of ending a gating of a receiving signal in a second embodiment of the invention,
Fig. 11 a time diagram of ending a gating of a receiving signal in a third embodiment of the invention,
Fig. 12 a time diagram of ending a gating of a receiving signal in a fourth embodiment of the invention and
Fig. 13 a time diagram of RF phase noise, of squelch signal and of DC component of the carrier in an inventive apparatus for gating a receiving signal.
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Firstly the inventive apparatus and the inventive method for gating a receiving signal are described on the basis of Fig. 3 and 4 of the drawing:
In the first step S10 of the inventive method for gating a receiving signal the sampled amplitudes m<sub>n</sub> and sampled phase φ<sub>η</sub> of the sampled receiving audio signal x<sub>n</sub> are determined in an converter 1 - typically a Cordic-unit - on the basis of the sampled real component Re{x״} and the sampled imaginary component Im{x<sub>n</sub>} of the complex receiving audio signal x<sub>n</sub> .
In the following step S20 of the inventive method sampled rectified phase noise p<sub>n</sub> is determined on the basis of the sample phases φ<sub>η</sub>. Firstly the phase difference Δφ<sub>η</sub> between a sampled phase φ<sub>η</sub> and its succeeding sampled phase φ<sub>η</sub>_<sub>χ</sub> is determined for each sampling point in a differentiating unit 3. Secondly the low frequency signal portions of the phase difference - caused by frequency offset and frequency drift of the carrier signal - are eliminated in a 4<sup>th</sup> order highpass filter 6 to obtain a phase difference Δφ<sub>η</sub> comprising only high frequency signal portions being phase noise p<sub>n</sub>. In a squaring unit 7 the phase noise p<sub>n</sub> is rectified. Alternatively the rectifying of the phase noise p can be performed by means of a absolute value performing unit.
In the next step S30 of the inventive method the squelch signal s<sub>n</sub> is determined by averaging the rectified phase noise p<sub>n</sub> in a digital filter 9 with proportional-integral characteristic.
Optionally in case of a rising squelch signal s<sub>n</sub> being below a selected higher threshold S<sub>hjgh</sub> the value of the squelch signal s<sub>n</sub> is changed to the higher threshold S<sub>high </sub>according to Fig. 13 in a gating unit 10. Consequently in case of a dropping squelch signal s<sub>n</sub> being higher a selected lower threshold S<sub>lnw</sub> the value of the squelch signal s<sub>n </sub>is changed to the lower threshold S<sub>low</sub> according to Fig. 13
G:\CP12K\Letter Module\LettersByUsers\P\2006\P30489\20061227_l657־_UU Unterlagen, uspriinglich_P30489_EP.c in the gate unit 10. By these means the time for starting resp. for ending the gating is thus reduced.
The following step S40 of the inventive method comprises the determination of the start point and of the end point of gating.
In a gating unit 10 the squelch signal s<sub>n</sub> is compared with a selected higher threshold S<sub>high</sub> in case of a rising of the squelch signal s<sub>n</sub>. The start point SP<sub>CA</sub> of gating in a first embodiment of the invention occurs according to Fig. 5, when the squelch signal s<sub>n</sub> rises above the higher threshold S<sub>high</sub> and a subsequent first delay time T<sub>D] </sub>expires. The starting of gating is characterised by the rising audio gate signal AG - the control signal for gating the amplitudes m<sub>n</sub> of the received audio signal in the gating unit 10 - in Fig. 5.
In a second embodiment of the invention the user of the receiver determines the start point SP<sub>G2</sub> of gating by adjusting the start point SP<sub>GX</sub> of gating of the first embodiment of invention, until phase noise disappears at the beginning of gating. The start point SP<sub>G2</sub> of the second embodiment of the invention corresponds to an adjustment of the start point SP<sub>G}</sub> of gating of the first embodiment of invention in the size of a first time interval Δζ according to Fig. 6. The adjustment in the size of a first time interval Δζ<sub>ρ</sub> can be performed in both directions relative to the start point SP<sub>Gl</sub> of gating of the first embodiment of invention.
In a third embodiment of the invention the gating is started from zero up to an active gating level inside a first fading time T<sub>fodel</sub> . Defining the start of fading as the start point of gating the start point SP<sub>G3</sub> of the third embodiment of the invention corresponds to the start point SP<sub>G2</sub> of gating of the second embodiment of invention according to Fig. 7.
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In a fourth embodiment of the invention the end of fading defines the start point of gating leading to a start point
SP<sub>(;4</sub> of the fourth embodiment of the invention according to Fig. 8.
For determining the end point of gating the dropping squelch signal s<sub>n</sub> is compared with a selected lower threshold S<sub>low</sub> in the gating unit 10. The end point EP<sub>GX</sub> of gating of the first embodiment of the invention occurs according to Fig. 9, when the squelch signal s<sub>n</sub> drops below the lower threshold S<sub>low</sub> and a subsequent second delay time T<sub>D2</sub> expires. The ending of gating is characterised by the dropping audio gate signal AG in Fig. 9.
In the second embodiment of the invention the end point׳ EP<sub>G2</sub> of gating is determined by adjusting the end point EP<sub>gx</sub> of gating of the first embodiment of the invention, until the phase noise disappears at the end of gating. The end point EP<sub>G2</sub> of the second embodiment of the invention corresponds to an adjustment of the end point EP<sub>GX</sub> of gating of the first embodiment of invention in the size of a second time interval Et<sub>ep</sub> according to Fig. 10.
In the third embodiment of the invention with fading from an active gating level down to zero inside a second fading time T<sub>fade2</sub> at the end of gating according to Fig. 11 the end point EP<sub>G2</sub> of gating corresponds to the end point EP<sub>G2 </sub>of the second embodiment of the invention, if the start of fading defines the end point of gating.
According to Fig. 12 the end point EP<sub>Gi:</sub> of gating in the fourth embodiment of the invention corresponds to the end point EP<sub>g2</sub> of the second embodiment of the invention in addition to the second fading time T<sub>fade2</sub>, if the end of fading defines the end point of gating.
In the following step S50 of the inventive method the third delay time T<sub>Di</sub> for delaying the sampled amplitudes m<sub>n</sub> of the received audio signal at the beginning of the
G:\CPI2K\Letler Moduie\LettersByUsers\P\2006\P30489\20061227_l6-57_UU Unterlagen, usprunglich_P30489_EP.c gating and the fourth delay time T<sub>M</sub> for delaying the sampled amplitudes m<sub>n</sub> of the received audio signal at the end of the gating are calculated.
The third delay time T<sub>D3</sub> at the beginning of the gating in the first embodiment of the invention calculates according to equation (2a):
(2a)
The third delay time T<sub>D3</sub> at the beginning of the gating in the second embodiment of the invention calculates according to equation (2b), whereby a positive value of the first time interval Δί corresponds to a start point SP<sub>G2 </sub>of gating of the second embodiment of invention being earlier than the rising of the squelch signal s<sub>n</sub> above the higher threshold S<sub>high</sub>:
T<sub>l)3</sub>>T<sub>m</sub>+Δί<sub>χρ</sub> (2b)
The third delay time T<sub>D3</sub> at the beginning of the gating in the third embodiment of the invention calculates according to equation (2c), whereby a positive value of the first time interval Δζ<sub>ρ</sub> corresponds to a start point SP<sub>G3</sub> of gating of the third embodiment of invention being earlier than the rising of the squelch signal s<sub>n</sub> above the higher threshold S<sub>high</sub> :
^03 - <sup>+</sup> Δϊ.φ (2 c)
The third delay time T<sub>D3</sub> at the beginning of the gating in the fourth embodiment of the invention calculates according to equation (2d), whereby a positive value of the first time interval Δζ<sub>ρ</sub> corresponds to a start point SP<sub>C4 </sub>of gating of the fourth embodiment of invention being earlier than the rising of the squelch signal s<sub>n</sub> above the higher threshold S<sub>high</sub> :
Td3 - Ρβ! <sup>+</sup> ^sp ~ I'fadel (2d)
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The fourth delay time T<sub>Di</sub> at the end of the gating in the first embodiment of the invention calculates according to equation (3a):
T >T <sup>J</sup> W4 - <sup>1</sup> D2 (3a)
The fourth delay time T<sub>D4</sub> at the end of the gating in the second embodiment of the invention calculates according to equation (3b), whereby a positive value of the second time interval Et corresponds to an end point EP<sub>G2</sub> of gating of the second embodiment of invention being earlier than the dropping of the squelch signal s<sub>n</sub> below the lower threshold S<sub>low</sub>׳.
^>4 - ^D2 <sup>+</sup> kt<sub>ep</sub> (3b)
The fourth delay time T<sub>D4</sub> at the end of the gating in the third embodiment of the invention calculates according to equation (3c), whereby a positive value of the second time interval Δζ<sub>ρ</sub> corresponds to an end point EP<sub>G3</sub> of gating of the third embodiment of invention being earlier than the dropping of the squelch signal s<sub>n</sub> below the lower threshold <sup>:</sup>
7.<sub>μ</sub>>7.<sub>0!</sub>+Δ<3) ״c)
The fourth delay time T<sub>D4</sub> at the end of the gating in the fourth embodiment of the invention calculates according to equation (3d), whereby a positive value of the second time interval Δ/ corresponds to an end point EP<sub>G4</sub> of gating of the fourth embodiment of invention being earlier than the dropping of the squelch signal s<sub>n</sub> below the lower threshold S<sub>low</sub>:
^04 - ^02 <sup>+</sup> At<sub>ep</sub> + Tf<sub>a</sub>de<sub>2</sub> (3d)
For delaying the sampled amplitudes m<sub>n</sub> of the received audio signal both at the beginning and also at the end of
G:\CPl2K\Letter Module\LettcrsByUsers\P\2006\P30489\2006l227_l6-57_UU Unterlagen, uspriinglich_P30489_EP.c the gating the maximum delay time T<sub>DMax</sub> is chosen of the third delay time Τ<sub>υ3</sub> at the beginning of the gating and of the fourth delay time T<sub>M</sub> at the end of the gating in the next step S60 according to equation (4):
T<sub>DMax</sub>=^{W<sub>D</sub>»T<sub>D4</sub>} (4)
In step S60 the sampled amplitudes m<sub>n</sub> of the received audio signal are delayed in a delay unit 12 located between the demodulator 9 and the gating unit 10 in the inventive apparatus for gating a received signal according to Fig. 3 with the maximum delay time T<sub>DMax</sub>.
The failure caused by choosing one delay time of the third delay time T<sub>D3</sub> or the fourth delay time T<sub>D4</sub> for the delay time T<sub>DMax</sub> applied for delaying the sampled amplitudes m<sub>n </sub>of the received audio signal both at the beginning and at the end of the gating is compensated in the next step S70 by recalculating the first delay time T<sub>DX</sub> and the second delay time T<sub>D2</sub> :
For the first embodiment of the invention the first delay T<sub>D]</sub> is recalculated according to equation (5a) and the second delay time T<sub>D2</sub> is recalculated according to equation (6a):
I'd] <sup>=</sup> ?DMax (5a)
I'd2<sup>=</sup>I'dmox (6a)
For the second embodiment of the invention the first delay T<sub>DX</sub> is recalculated according to equation (5b) and the second delay time T<sub>D2</sub> is recalculated according to equation (6b):
77, = T<sub>I)M</sub>״ - ΔΓ״
DI DM ax sp
I'd! ~ Idmox At<sub>ep</sub> (5b) (6b)
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For the third embodiment of the invention the first delay T<sub>D</sub>\ is recalculated according to equation (5c) and the second delay time T<sub>D2</sub> is recalculated according to equation (6c):
<sup>=</sup> ~ At,ip ( 5 C ) ^D1 ~ T-DMax. ~ At<sub>ep</sub> ( 60 )
For the fourth embodiment of the invention the first delay T<sub>D}</sub> is recalculated according to equation (5d) and the second delay time Τ<sub>ϋ2</sub> is recalculated according to equa¾., tion (6d):
= T<sub>DM!a</sub> — Et<sub>xp</sub> -i-1 j-<sub>M</sub> (5d) ?!)2 <sup>=</sup> ΤβΜαχ ~ <sub>ep</sub> ־־־ Tj-<sub>ade2</sub> ( 6 d)
By using the recalculated first delay time according 20 to one of the equations (5a) to (5d) and the second delay time T<sub>D2</sub> according to one of the equations (6a) to (6d) the new start point SP<sub>G3</sub>, SP<sub>G2</sub>, SP<sub>G3</sub> or SP<sub>Gi</sub> of the first, second, third or fourth embodiment of the invention according to Fig. 5, 6, 7 or 8 and the end point EP<sub>G}</sub>, 25 EP<sub>G2</sub>,EP<sub>G3</sub> or EP<sub>GA</sub> of the first, second, third or fourth
Τ' embodiment of the invention according to Fig. 9, 10, 11 or is determined in the next step S80.
In the last step S90 of the inventive method the delayed 30 sampled amplitudes m<sub>n</sub> of the received audio signal are gated in the gating unit 10 between the start point
SP<sub>CX</sub> , SP<sub>G2</sub>, SP<sub>G3</sub> or SP<sub>C4</sub> in the first, second, third or fourth embodiment of the invention and the end point EP<sub>G{</sub>, EP<sub>G2</sub>, EP<sub>G3</sub> or EP<sub>ga</sub> of the first, second, third or fourth embo35 diment of the invention.
The invention is not limited to the embodiment of the inventive apparatus and to the four embodiments of the inventive method for gating a receiving signal. The invenG:\CPI2K\Letter Module\LcttersByUsers\P\2006\P30489\2006l227_l6-57_UU Unterlagen, usprtjnglich P30489_EP.c tion also covers other combinations of the embodiments of the inventive method, for example a level and time trigger of the squelch signal s<sub>n</sub> without using any user specific adjustment of the start point and/or end point of gating in combination with fading of the gating. Furthermore, nonlinear characteristic of fading - for example a squared fading characteristic - is also inside the scope of the invention.
10 sheets
Sheet 1 Sheet 2 Sheet 3 Sheet 4 Sheet 5 Sheet 6 Sheet 7 Sheet 8 Sheet 9 Sheet 10
13 members in 4 offices
Priority claims8
| Document | Office | Kind | Date |
|---|---|---|---|
| 06007405 | European Patent Office (EPO) | A | |
| 06007405 | European Patent Office (EPO) | A | |
| 07000145 | European Patent Office (EPO) | A | |
| 07000145 | European Patent Office (EPO) | A | |
| 060074051 | – | – | – |
| 070001458 | – | – | – |
| EP20060007405 | – | – | – |
| EP20070000145 | – | – | – |
Members13
| Document | Office | Kind | |
|---|---|---|---|
| IL182301A0 | Israel | A0 | |
| EP1843466A1 | European Patent Office (EPO) | A1 | |
| EP1843467A2 | European Patent Office (EPO) | A2 | |
| US2007275678A1 | United States of America | A1 | |
| US2007275685A1 | United States of America | A1 | |
| EP1843466B1 | European Patent Office (EPO) | B1 | |
| DE602006002960D1 | Germany | D1 | |
| EP1843467A3 | European Patent Office (EPO) | A3 | |
| EP1843467B1 | European Patent Office (EPO) | B1 | |
| US7734268B2 | United States of America | B2 | |
| DE602007006710D1 | Germany | D1 | |
| US7907923B2 | United States of America | B2 | |
| IL182301AThis record | Israel | A |
5 legal events, as the office reported them to INPADOC
Over the term
Point at a mark for the eventEvents
| Event | Code | |
|---|---|---|
| Patent renewedKB | KB | |
| Patent renewedKB | KB | |
| Patent renewedKB | KB | |
| Patent renewedKB | KB | |
| Patent grantedGrantedFF | FF |
Numbers
- Publication, DOCDB
- 182301
- Publication, EPODOC
- IL182301
- Application
- 182301
- Application, DOCDB
- 18230107
- Application, EPODOC
- IL20070182301
Titles
- English
- METHOD AND APPARATUS FOR SQUELCH GATING A RECEIVING SIGNAL
Classification
- CPC, 1
- H03G3/344
